Full text: Théorie générale des orbites absolues (Tome 1)

Première Partie. Livre II. 
105 
avoir remplacé 
notations 
#i par U -f- il — 0 et par }>■ -f- U' — 0' et, adopté les 
ft — ty = b\ & — 0' = ÿ. 
Azoici les termes dont il s’agit: 
COS II = il — - P — - T 2 j cos (v — v') 
14 4 ! v ' 
+ ~ 7 2 COS (v -f v' 2 # 2 (Âf 0 j) 
+ ^ J' 2 COS (v -f v' 2ÏÏ 2 (il' 0 ')) 
+ l - IV cos (v v' (b — b') — (il — 0 ) + il' — 0 ') 
— l - IV cos (v -f v' — (b + b') — (il — 0 ) — (il’ — 0 ')), 
COS 2 H=— 1 -P—-r i 
2 2 
+ {l -ir_i J T'*jcOS2(v-Y') 
+ P COS ( 2 V 2 Ï} 2 (il 0 )) 
+ 2 ^ ,2 cos ( 2V 2ÿ 2(û' 0')) 
■ 1 
+ “ V 2 COS ( 2 V' 2 $ 2(12 0 )) 
+ ^ I' 2 COS ( 2 V' 2 #' 2 (il’ 0 ')) 
+ IV COS(2(v — v') — (b — b) — (il — 0 ) + il' — 0 ') . 
— IV COS (2 V — $ + ¿0 — (& — 0 ) — (XT — 0 ')) 
— ir cos(2v' — (b + b') — (il — O) — (il' — 0')) 
-f -IV cos ($ — # -f- il — 0 — (il 0 )), 
I
	        
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